In recent work, several academic groups, including ours, have
demonstrated optical-interconnect systems in the lab [12-26]. Due to the challenges and cost of implementing large
scale fiber systems, these have
tended to be free-space interconnects.
The primary differences between the
various projects have tended to be in two areas: the choice of optoelectronic devices – lasers or modulators, p-i-n or metal-semiconductor-
metal (MSM) detectors – and the design of the optical system itself.
Since this thesis deals with the question
of optoelectronic modulators,
a discussion of the advantages and disadvantages of a VCSEL-based approach will appear in Chapter
3. Let us briefly
describe some recent representative examples of the academic groups’ work on optical- interconnect systems. (A more exhaustive review is given in a few recent published special issue journals [27, 28].)
The Esener Group at University of California at San Diego has designed
and demonstrated an optical interconnect system with silicon chips mounted on a PCB as
usual [14]. On top of the chips, a 4-f imaging system was
implemented in commercially- available bulk macro-optics. As a test
system,
this
project
was
able to show the feasibility of combining multiple types of materials, such as Si, GaAs VCSELs and MSMs,
ceramics, glass
lenses and mirrors, PCBs, etc.,
and of achieving
a working system. Future
systems would be expected to use microlenses
instead, in order to reduce cost
and improve scalability.
The advantage
of this scheme
is its use of currently available products in a relatively compact
design. Drawbacks
are that it is still a bit too
bulky for practical use and the published speed of 250 MHz is far too low.
Of course, this would improve as CMOS
technology improves and the optical system is not sensitive to the bit rate. The scalability of a system with bulk
optics is also an unresolved question.
The work of Jurgen Jahns and Matthias Gruber in planar optics has the potential to solve this problem of
the scalability of optics [24, 25, 29, 30]. Using
a glass substrate, diffractive optical
elements (DOEs) can be etched into
the surface. CMOS
chips can then be flip-chip
bonded with high accuracy onto this glass substrate. Routing of electrical signals and power lines could be achieved by running wires along the glass
surface, as well. Diffractive optical systems are able to perform
more complicated routing
functions, instead of relying on simple bulk optics to perform the same function to the entire array
of signals. This technology can also be integrated with standard PCBs and fiber-based
optics as shown below.
Fig. 2.1. Planar
optics of Jahns
and
Gruber (image courtesy
M. Gruber)
The group of Hugo Thienpont
has also been investigating microoptical systems
[13, 17]. Their work in materials
such as polymethylmethacrylate (PMMA) using the technique of deep proton lithography has
yielded high quality results,
especially for intrachip or short distance intra-MCM optical interconnects. Such short distance interconnects may be useful
for signaling as well as clock
distribution.
Finally, the Miller group has utilized bulk optics to design a free-space optical interconnects test system [20, 22, 31]. The purpose was not to study packaging technology, but instead to characterize important system parameters in optical
interconnects and to demonstrate the
benefits of using certain schemes. Using a short- pulse modelocked
laser as the
light source, we demonstrated
improved receiver sensitivity [20, 32, 33], optical
link latency reduction [31, 32], and WDM optical
interconnects using spectral
slicing [22]. The issue of clock distribution was also addressed using several schemes, including the so-called “receiver-less” design [20, 33,
34]. Many
of these results
would apply equally well to the integrated planar optical systems
being studied by Jahns and Gruber, for example.
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